Silicon carbide semiconductor substrate, method of manufacturing silicon carbide semiconductor substrate, semiconductor device, and method of manufacturing semiconductor device

ABSTRACT

A silicon carbide semiconductor substrate includes a silicon carbide substrate of a first conductivity type, an epitaxial layer of the first conductivity type provided on a front surface of the silicon carbide substrate, an impurity concentration of the epitaxial layer being 1×1017/cm3 to 1×1018/cm3, and a film thickness of the epitaxial layer being 1 μm to 5 μm. The silicon carbide semiconductor substrate further includes a buffer layer of the first conductivity type provided on a surface of a first side of the epitaxial layer opposite a second side facing the silicon carbide substrate, an impurity concentration of the buffer layer being about a same as that of the silicon carbide substrate, and a drift layer of the first conductivity type provided on a surface of a first side of the buffer layer opposite a second side facing toward the silicon carbide substrate, an impurity concentration of the drift layer being lower than that of the buffer layer.

CROSS REFERENCE TO RELATED APPLICATIONS

This is a continuation application of International Application PCT/JP2016/087389 filed on Dec. 15, 2016 which claims priority from a Japanese Patent Application Nos. 2015-247955 filed on Dec. 18, 2015, and 2016-150855 filed on Jul. 29, 2016, the contents of which are incorporated herein by reference.

BACKGROUND OF THE INVENTION 1. Field of the Invention

Embodiments of the invention relate to a silicon carbide semiconductor substrate, a method of manufacturing a silicon carbide semiconductor substrate, a semiconductor device, and a method of manufacturing a semiconductor device.

2. Description of the Related Art

An epitaxial wafer (silicon carbide semiconductor substrate, hereinafter, simply, substrate) in which silicon carbide (SiC) is formed on a substrate by epitaxial growth contains many crystal defects/dislocations and these crystal defects/dislocations are thought to adversely affect the properties of the silicon carbide semiconductor device. In particular, basal plane dislocations (BPDs) in a layer formed by epitaxial growth expand to stacked defects with bipolar operation of the semiconductor device whereby the flow of current becomes difficult, thereby increasing the ON voltage of the semiconductor device and leading to bipolar degradation.

BPDs are present in the substrate at a density of several hundred to several thousand/cm². Many of the BPDs are converted into threading edge dislocations (TED) during epitaxial growth. Nonetheless, after the epitaxial growth, BPDs remain in the substrate at a density of 1 to 100/cm². In this state, when excessive current flows with bipolar operation of a silicon carbide semiconductor device produced (manufactured) from the substrate, BPDs in the substrate expand whereby triangular/bar-shaped stacking faults are generated.

FIG. 6 is a top view schematic of photographed photoluminescence of stacking faults occurring in a conventional silicon carbide semiconductor substrate. FIG. 6 depicts results of photoluminescence measurements performed with respect to a substrate at room temperature by using a bandpass filter in the vicinity of 420 nm after about 1 hour of bipolar operation of a pin (p-intrinsic-n) diode at a current density of 600 A/cm² and peeling of the anode electrode, the pin diode being formed from the conventional silicon carbide semiconductor substrate. In FIG. 6, in the substrate, light emitting states of both a long, bar-shaped stacking fault extending between left and right ends of the substrate and multiple triangular-shaped stacking faults are shown.

Factors causing the bar-shaped stacking fault and the triangular-shaped stacking faults include electron-hole recombination. To suppress this recombination, there is a technique that prevents excessive hole injection to the substrate by forming a thick buffer layer on the substrate by epitaxial growth (hereinafter, epi growth) (e.g., refer to J. J. Sumakeris, et al, “Approaches to Stabilizing the Forward Voltage of Bipolar SiC Devices”, (USA), Materials Science Forum, On-line Vol. 457-460, 2004, pp. 1113-1116).

SUMMARY OF THE INVENTION

According to one embodiment of the invention, a silicon carbide semiconductor substrate includes a silicon carbide substrate of a first conductivity type; an epitaxial layer of the first conductivity type provided on a front surface of the silicon carbide substrate, an impurity concentration of the epitaxial layer being 1×10¹⁷/cm³ to 1×10¹⁸/cm³, and a film thickness of the epitaxial layer being 1 μm to 5 μm; a buffer layer of the first conductivity type provided on a surface of a first side of the epitaxial layer opposite a second side facing the silicon carbide substrate, an impurity concentration of the buffer layer being about a same impurity concentration as that of the silicon carbide substrate; and a drift layer of the first conductivity type provided on a surface of a first side of the buffer layer opposite a second side facing toward the silicon carbide substrate, an impurity concentration of the drift layer being lower than that of the buffer layer.

In the embodiment, the impurity concentration of the buffer layer is 3 times the impurity concentration of the epitaxial layer or more, and a thickness of the buffer layer is 3 μm or more.

According to another embodiment of the invention, a method of manufacturing a silicon carbide semiconductor substrate includes forming, on a front surface of a silicon carbide substrate, an epitaxial layer of a first conductivity type, an impurity concentration of the epitaxial layer being 1×10¹⁷/cm³ to 1×10¹⁸/cm³, and a film thickness of the epitaxial layer being 1 μm to 5 μm; forming a buffer layer of the first conductivity type on a surface of a first side of the epitaxial layer opposite a second side facing the silicon carbide substrate, an impurity concentration of the buffer layer being about a same impurity concentration as that of the silicon carbide substrate; and forming a drift layer of the first conductivity type on a surface of a first side of the buffer layer opposite a second side facing toward the silicon carbide substrate, an impurity concentration of the buffer layer being lower than that of the buffer layer.

In the embodiment, the impurity concentration of the buffer layer is 3 times the impurity concentration of the epitaxial layer or more, and a thickness of the buffer layer is 3 μm or more.

According to another embodiment of the invention, a semiconductor device includes a silicon carbide semiconductor substrate that includes a silicon carbide substrate of a first conductivity type; an epitaxial layer of the first conductivity type provided on a front surface of the silicon carbide substrate, an impurity concentration of the epitaxial layer being 1×10¹⁷/cm³ to 1×10¹⁸/cm³, and a film thickness of the epitaxial layer being 1 μm to 5 μm; a buffer layer of the first conductivity type provided on a surface of a first side of the epitaxial layer opposite a second side facing the silicon carbide substrate, an impurity concentration of the buffer layer being about a same impurity concentration as that of the silicon carbide substrate; and a drift layer of the first conductivity type provided on a surface of a first side of the buffer layer opposite a second side facing toward the silicon carbide substrate, an impurity concentration of the drift layer being lower than that of the buffer layer.

In the embodiment, the impurity concentration of the buffer layer is 3 times the impurity concentration of the epitaxial layer or more, and a thickness of the buffer layer is 3 μm or more.

According to another embodiment of the invention, a method of manufacturing a semiconductor device includes using a silicon carbide semiconductor substrate that includes a silicon carbide substrate of a first conductivity type; an epitaxial layer of the first conductivity type provided on a front surface of the silicon carbide substrate, an impurity concentration of the epitaxial layer being 1×10¹⁷/cm³ to 1×10¹⁸/cm³, and a film thickness of the epitaxial layer being 1 μm to 5 μm; a buffer layer of the first conductivity type provided on a surface of a first side of the epitaxial layer opposite a second side facing the silicon carbide substrate, an impurity concentration of the buffer layer being about a same impurity concentration as that of the silicon carbide substrate; and a drift layer of the first conductivity type provided on a surface of a first side of the buffer layer opposite a second side facing toward the silicon carbide substrate, an impurity concentration of the drift layer being lower than that of the buffer layer.

In the embodiment, the impurity concentration of the buffer layer is 3 times the impurity concentration of the epitaxial layer or more, and a thickness of the buffer layer is 3 μm or more.

Objects, features, and advantages of the present invention are specifically set forth in or will become apparent from the following detailed description of the invention when read in conjunction with the accompanying drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a cross-sectional view of a silicon carbide semiconductor substrate according to an embodiment;

FIG. 2 is a diagram of infrared light reflection of the silicon carbide semiconductor substrate according to the embodiment;

FIG. 3 is a graph schematically depicting FT-IR interference waveforms of the silicon carbide semiconductor substrate according to the embodiment;

FIG. 4 is a table of impurity concentrations and thicknesses of each layer in examples of the silicon carbide semiconductor substrate according to the embodiment;

FIGS. 5A, 5B, 5C, and 5D are graphs of a FT-IR signal in the examples of the silicon carbide semiconductor substrate according to the embodiment;

FIG. 6 is a top view schematic of photographed photoluminescence of stacking faults occurring in a conventional silicon carbide semiconductor substrate;

FIG. 7 is a cross-sectional view of the stacking-fault-suppressing semiconductor substrate;

FIG. 8 is a diagram of infrared light reflection of the stacking-fault-suppressing semiconductor substrate; and

FIG. 9 is a graph schematically depicting Fourier Transform Infrared Spectroscopy (FT-IR) of the stacking-fault-suppressing semiconductor substrate.

DETAILED DESCRIPTION OF THE INVENTION

With conventional techniques, formation of a thick buffer layer leads to increased cost due to decreased epi growth throughput, decreased yield due to increased defect density, and increased substrate resistance. In this regard, one conventional silicon carbide semiconductor substrate (hereinafter, stacking-fault-suppressing semiconductor substrate) has been proposed in which the buffer layer is formed to have an impurity concentration that is about the same as that of the substrate whereby the thickness of the buffer layer may be suppressed, enabling the stacking-fault-suppressing semiconductor substrate to effectively suppress the occurrence of triangular/bar-shaped stacking faults in the substrate even when bipolar operation is performed using large current.

FIG. 7 is a cross-sectional view of the stacking-fault-suppressing semiconductor substrate. As depicted in FIG. 7, in a stacking-fault-suppressing substrate, an n⁺-type silicon carbide buffer layer 102 is deposited on a first main surface (front surface), for example, a (0001) plane (Si face) of an n⁺-type silicon carbide substrate 101.

The n⁺-type silicon carbide substrate 101 is a silicon carbide, single crystal substrate doped with, for example, nitrogen (N). The n⁺-type silicon carbide buffer layer 102 is a buffer layer doped with, for example, nitrogen and has an impurity concentration that is about the same as that of the n⁺-type silicon carbide substrate 101. On a surface side of the n⁺-type silicon carbide buffer layer 102 opposite the side facing the n⁺-type silicon carbide substrate 101, an n-type drift layer 103 is formed. The n-type drift layer 103 is a drift layer doped with, for example, nitrogen and has an impurity concentration that is lower than that of the n⁺-type silicon carbide substrate 101 and that of the n⁺-type silicon carbide buffer layer 102.

The stacking-fault-suppressing semiconductor substrate promotes electron-hole recombination in the n⁺-type silicon carbide buffer layer 102 and suppresses the hole density injected into the n⁺-type silicon carbide substrate 101 to thereby effectively suppress the occurrence of triangular/bar-shaped stacking faults.

Nonetheless, in the stacking-fault-suppressing semiconductor substrate, the impurity concentrations of the n⁺-type silicon carbide substrate 101 and the n⁺-type silicon carbide buffer layer 102 are about the same and therefore, the reflection of infrared light by an interface of the n⁺-type silicon carbide substrate 101 and the n⁺-type silicon carbide buffer layer 102 decreases.

FIG. 8 is a diagram of infrared light reflection of the stacking-fault-suppressing semiconductor substrate. As depicted in FIG. 8, infrared rays incident on the stacking-fault-suppressing semiconductor substrate are reflected by the surface of the stacking-fault-suppressing semiconductor substrate and returned as surface reflected light Ref. Because the impurity concentrations of the n⁺-type silicon carbide buffer layer 102 and the n-type drift layer 103 differ, the infrared rays are reflected by an interface of the n⁺-type silicon carbide buffer layer 102 and the n-type drift layer 103 and are returned as interface reflected light C. However, since the impurity concentrations of the n⁺-type silicon carbide substrate 101 and the n⁺-type silicon carbide buffer layer 102 are about the same, the interface reflected light is minimally reflected by the interface of the n⁺-type silicon carbide substrate 101 and the n⁺-type silicon carbide buffer layer 102 and thus, the interface reflected light is not returned.

FIG. 9 is a graph schematically depicting Fourier Transform Infrared Spectroscopy (FT-IR) of the stacking-fault-suppressing semiconductor substrate. The horizontal axis represents film thickness and the vertical axis represents the FT-IR signal spectrum. As depicted in FIG. 9, an interference waveform of the stacking-fault-suppressing semiconductor substrate is only the interference waveform (Ref.+C) of the interface reflected light C from the interface of the n⁺-type silicon carbide buffer layer 102 and the n-type drift layer 103, and the surface reflected light Ref. since there is no interface reflected light from the interface of the n⁺-type silicon carbide substrate 101 and the n⁺-type silicon carbide buffer layer 102. Therefore, the film thickness of the n⁺-type silicon carbide buffer layer 102 cannot be measured. Thus, as described, a problem arises in that in the stacking-fault-suppressing semiconductor substrate, the film thickness of the n⁺-type silicon carbide buffer layer 102 cannot be measured by a conventional FT-IR method (Fourier Transform Infrared Spectroscopy). Further, since the film thickness of the buffer layer 2 cannot be measured accurately, the problems of decreased yield of the silicon carbide semiconductor substrate and increased substrate resistance cannot be resolved.

Embodiments of a silicon carbide semiconductor substrate, a method of manufacturing a silicon carbide semiconductor substrate, a semiconductor device, and a method of manufacturing a semiconductor device according to the present invention will be described in detail with reference to the accompanying drawings. In the present description and accompanying drawings, layers and regions prefixed with n or p mean that majority carriers are electrons or holes. Additionally, + or − appended to n or p means that the impurity concentration is higher or lower, respectively, than layers and regions without + or −. Cases where symbols such as n's and p's that include + or − are the same indicate that concentrations are close and therefore, the concentrations are not necessarily equal. In the description of the embodiments below and the accompanying drawings, main portions that are identical will be given the same reference numerals and will not be repeatedly described. Further, in the present description, when Miller indices are described, “−” means a bar added to an index immediately after the “−”, and a negative index is expressed by prefixing “−” to the index.

FIG. 1 is a cross-sectional view of a silicon carbide semiconductor substrate according to an embodiment. As depicted in FIG. 1, in the silicon carbide semiconductor substrate according to the embodiment, an n-type epitaxial layer (epitaxial layer of a first conductivity type) 4 is deposited on a first main surface (front surface), e.g., (0001) plane (Si face), of an n⁺-type silicon carbide substrate (silicon carbide substrate of the first conductivity type) 1.

The n⁺-type silicon carbide substrate 1, for example, is a silicon carbide, single crystal substrate doped with nitrogen. An impurity concentration of the n⁺-type silicon carbide substrate 1 is, for example, 1×10¹⁸/cm³ or higher, 2×10¹⁹/cm³ or less. The n-type epitaxial layer 4 has an impurity concentration that is lower than that of the n⁺-type silicon carbide substrate 1 and lower than that of an n⁺-type silicon carbide buffer layer (buffer layer of the first conductivity type) 2 described hereinafter. The n-type epitaxial layer 4 is an epitaxial layer doped with, for example, nitrogen. Further, an impurity concentration of the n-type epitaxial layer 4 may be ⅓ or less of the impurity concentration of the n⁺-type silicon carbide substrate 1 or ⅓ or less of the impurity concentration of the n⁺-type silicon carbide buffer layer 2. As described in detail below, the reason for this is that at an interface of the n⁺-type silicon carbide substrate 1 and the n-type epitaxial layer 4 or an interface of the n⁺-type silicon carbide buffer layer 2 and the n-type epitaxial layer 4, interface reflected light necessary for measuring the film thickness of the n⁺-type silicon carbide buffer layer 2 is obtained. Further, the film thickness of the n-type epitaxial layer 4 may be less than 5 μm because when the film thickness is too thick, the resistance increases due to the n-type epitaxial layer 4. The impurity concentration of the n-type epitaxial layer 4 may be 1×10¹⁷/cm³ or higher because when the impurity concentration is too low, the resistance increases due to the n-type epitaxial layer 4.

Here, the impurity concentration of the n-type epitaxial layer 4 may be 1×10¹⁸/cm³ or less, and the film thickness of the n-type epitaxial layer 4 may be 1 μm or more. As a result, it becomes possible to detect basal plane dislocations occurring in the n-type epitaxial layer 4 using fluorescence by photoluminescence.

Here, from the experience of the inventors, in order to detect basal plane dislocations with high contrast by photoluminescence, a sufficient amount of free carriers has to be present. However, when a layer having a high impurity concentration is provided like in a conventional device, a non-radiative recombination process becomes dominant in the layer whereby the amount of carriers necessary for the luminescence of the basal plane dislocations cannot be secured, making detection of basal plane dislocations difficult.

In contrast, in the present invention, the n-type epitaxial layer 4 having a low concentration is provided whereby it becomes possible to detect generated basal plane dislocations by fluorescence. Therefore, it becomes possible to detect and remove elements in which stacking faults have a possibility of occurring, whereby inspections conventionally performed after manufacturing may be omitted, enabling reductions in cost.

On a surface side of the n-type epitaxial layer 4 opposite the side facing the n⁺-type silicon carbide substrate 1, the n⁺-type silicon carbide buffer layer 2 is provided. The n⁺-type silicon carbide buffer layer 2 is a buffer layer doped with, for example, nitrogen and has an impurity concentration that is about the same as that of the n⁺-type silicon carbide substrate 1. On a surface side of the n⁺-type silicon carbide buffer layer 2 opposite the side facing the n⁺-type silicon carbide substrate 1, an n-type drift layer (drift layer of the first conductivity type) 3 is formed. The n-type drift layer 3 is a drift layer doped with, for example, nitrogen and has an impurity concentration that is lower than that of the n⁺-type silicon carbide substrate 1 and that of the n⁺-type silicon carbide buffer layer 2.

A method of manufacturing a silicon carbide semiconductor substrate according to the embodiment will be described. First, the n⁺-type silicon carbide substrate 1 containing silicon carbide of an n-type is prepared. The n⁺-type silicon carbide substrate 1 is, for example, a silicon carbide, single crystal substrate having an impurity concentration of 5×10¹⁸/cm³. On the first main surface of the n⁺-type silicon carbide substrate 1, the n-type epitaxial layer 4 containing silicon carbide is formed by epitaxial growth to have a thickness of, for example, about 5 μm while an n-type impurity, e.g., nitrogen atoms, is doped. The dose at the time of ion implantation for forming the n-type epitaxial layer 4 may set to be such that, for example, the impurity concentration becomes about 1×10¹⁸/cm³.

Next, on a surface of the n-type epitaxial layer 4, the n⁺-type silicon carbide buffer layer 2 is formed by epitaxial growth to have a thickness of, for example, about 30 μm while an n-type impurity, e.g., nitrogen atoms, is doped. The dose at the time of ion implantation for forming the n⁺-type silicon carbide buffer layer 2 may be set such that, for example, the impurity concentration becomes about 5×10¹⁸/cm³. As a result, the impurity concentration of the n⁺-type silicon carbide buffer layer 2 becomes about the same as the impurity concentration of the n⁺-type silicon carbide substrate 1. The impurity concentration of the n⁺-type silicon carbide buffer layer 2 may be 1×10¹⁸/cm³ to 2×10¹⁹/cm³. The impurity concentration of the n⁺-type silicon carbide buffer layer 2 is 7×10¹⁸/cm³ or higher and the thickness is 3 μm or more, whereby even when the impurity concentration of the n-type epitaxial layer 4 is low, stacking faults are suppressed.

Next, on the surface of the n⁺-type silicon carbide buffer layer 2, the n-type drift layer 3 is formed by epitaxial growth to have a thickness of, for example, about 10 μm while an n-type impurity, e.g., nitrogen atoms, is doped. The dose at the time of ion implantation for forming the n-type drift layer 3 may be set such that, for example, the impurity concentration becomes about 1×10¹⁶/cm³. As described, the silicon carbide semiconductor substrate depicted in FIG. 1 is completed.

FIG. 2 is a diagram of infrared light reflection of the silicon carbide semiconductor substrate according to the embodiment. As depicted in FIG. 2, infrared rays incident on the silicon carbide semiconductor substrate according to the embodiment are reflected by the surface of the silicon carbide semiconductor substrate and returned as surface reflected light Ref. Further, because the impurity concentrations of the n⁺-type silicon carbide substrate 1 and the n-type epitaxial layer 4 differ, the infrared rays are reflected by the interface of the n⁺-type silicon carbide substrate 1 and the n-type epitaxial layer 4 and are returned as interface reflected light A. Because the impurity concentrations of the n-type epitaxial layer 4 and the n⁺-type silicon carbide buffer layer 2 differ, the infrared rays are reflected by the interface of the n-type epitaxial layer 4 and the n⁺-type silicon carbide buffer layer 2 and are returned as interface reflected light B. Because the impurity concentrations of the n⁺-type silicon carbide buffer layer 2 and the n-type drift layer 3 differ, the infrared rays are reflected by the interface of the n⁺-type silicon carbide buffer layer 2 and the n-type drift layer 3 and returned as the interface reflected light C.

FIG. 3 is a graph schematically depicting FT-IR interference waveforms of the silicon carbide semiconductor substrate according to the embodiment. The horizontal axis represents film thickness and the vertical axis represents FT-IR signal spectrum. As depicted in FIG. 3, of the FT-IR interference waveforms of the silicon carbide semiconductor substrate according to the embodiment, interference waveform (Ref.+A) of the surface reflected light Ref. and the interface reflected light A, interference waveform (Ref.+B) of the surface reflected light Ref. and the interface reflected light B, and interference waveform (Ref.+C) of the surface reflected light Ref. and the interface reflected light C are measured. Thus, it becomes possible to measure the film thickness of the n⁺-type silicon carbide buffer layer 2 by Fourier transform from the interference waveform of the surface reflected light Ref. and the interface reflected light B and the interference waveform of the surface reflected light Ref. and the interface reflected light C.

FIG. 4 is a table of impurity concentrations and thicknesses of each layer in examples of the silicon carbide semiconductor substrate according to the embodiment. In the example, the impurity concentration and the thickness of the n⁺-type silicon carbide substrate 1 (in FIG. 4, indicated as substrate) are fixed at 5.0×10¹⁸/cm³ and 350 μm, respectively. Further, the impurity concentration and the thickness of the n-type epitaxial layer 4 (in FIG. 4, indicated as epi layer) are fixed at 1.0×10¹⁸/cm³ and 1 μm, respectively. The thickness of the n⁺-type silicon carbide buffer layer 2 (in FIG. 4, indicated as buffer layer) is fixed at 30 μm and the impurity concentration is varied.

Here, the impurity concentration of the n⁺-type silicon carbide buffer layer 2 was 1.0×10¹⁸/cm³ in example A, 3.0×10¹⁸/cm³ in example B, 5.0×10¹⁸/cm³ in example C, and 8.5×10¹⁸/cm³ in example D. In this manner, the ratio of the impurity concentration of the n⁺-type silicon carbide buffer layer 2 and the impurity concentration of the n-type epitaxial layer 4 was set to be 1 in example A, 3 in example B, 5 in example C, and 8.5 in example D.

FIGS. 5A, 5B, 5C, and 5D are graphs of a FT-IR signal in the examples of the silicon carbide semiconductor substrate according to the embodiment. The horizontal axis represents film thickness and the vertical axis represents FT-IR signal spectrum. The units are μm and percent, respectively. In example A, the impurity concentration of the n⁺-type silicon carbide buffer layer 2 and the impurity concentration of the n-type epitaxial layer 4 are about the same and therefore, only interference waveform A1 of the surface reflected light Ref. and interface reflected light C is measured. Interference waveform A1 corresponds to Ref.+C in FIG. 3. Therefore, in example A, the film thickness of the n⁺-type silicon carbide buffer layer 2 cannot be measured.

Meanwhile, in example B, the ratio of the impurity concentration of the n⁺-type silicon carbide buffer layer 2 and the impurity concentration of the n-type epitaxial layer 4 is 3 and the impurity concentrations differ. Therefore, interference waveform B1 of the surface reflected light Ref. and the interface reflected light C, and interference waveform B2 of the surface reflected light Ref. and the interface reflected light A, B are measured. Interference waveform B1 corresponds to Ref.+C in FIG. 3, and interference waveform B2 corresponds to Ref.+A and Ref.+B in FIG. 3. Here, since the n-type epitaxial layer 4 is thin, the interference waveform of the surface reflected light Ref. and the interface reflected light A and the interference waveform of the surface reflected light Ref. and the interface reflected light B are measured as the same interference waveform. Therefore, in example B, the film thickness of the n⁺-type silicon carbide buffer layer 2 may be measured from interference waveform B1 and interference waveform B2.

Similarly, in examples C and D, the ratios of the impurity concentration of the n⁺-type silicon carbide buffer layer 2 and the impurity concentration of the n-type epitaxial layer 4 are 5 and 8.5, respectively and the impurity concentrations differ. Therefore, interference waveforms C1, D1 of the surface reflected light Ref. and the interface reflected light C; and interference waveforms C2, D2 of the surface reflected light Ref. and the interface reflected light A, B are measured. Thus, in examples C and D, the film thickness of the n⁺-type silicon carbide buffer layer 2 may be measured from interference waveforms C1, D1, and interference waveforms C2, D2.

In this manner, from the examples, it is found that when the ratio of the impurity concentration of the n⁺-type silicon carbide buffer layer 2 and the impurity concentration of the n-type epitaxial layer 4 is 3 times or more, FT-IR signals are separated, enabling the film thickness of the n⁺-type silicon carbide buffer layer 2 to be evaluated. Further, from these results, it is found that when the ratio of the impurity concentration of the n⁺-type silicon carbide substrate 1 and the impurity concentration of the n-type epitaxial layer 4 is 3 times or greater, the FT-IR signals are separated, enabling the film thickness of the n⁺-type silicon carbide buffer layer 2 to be measured by Fourier transform.

A case in which a pin diode is manufactured from the silicon carbide semiconductor substrate according to the embodiment will be described as an example. For example, in a case where the silicon carbide semiconductor substrate according to the embodiment is an n-type and an n-channel pin diode is manufactured, the n⁺-type silicon carbide substrate 1 is a cathode region, the n⁺-type silicon carbide buffer layer 2 functions as a buffer layer, and the n-type drift layer 3 functions as an intrinsic semiconductor (i-layer). First, in a surface layer on a side of the n-type drift layer 3 opposite the side facing the n⁺-type silicon carbide buffer layer 2, a p-type impurity, for example, aluminum (Al) is ion implanted, whereby a p⁺-type anode region is formed. Next, on an upper surface of the anode region, an anode electrode is formed using nickel (Ni) or the like, and on an upper surface of the cathode region, a cathode electrode is formed. As a result, the n-channel pin diode is manufactured.

Here, for example, the impurity concentration of the n-type epitaxial layer 4 is 1/100 or less of the impurity concentration of the n-type drift layer 3 and the film thickness of the n-type epitaxial layer 4 is 1/10 or less of the film thickness of the n-type drift layer 3. As a result, the resistance of the n-type epitaxial layer 4 becomes 1/1000 or less of the resistance of the n-type drift layer 3. Therefore, the n-type epitaxial layer 4 does not become a large component of the resistance and does not negatively affect the performance of n-channel pin diode in a significant way.

Further, here, although an n-channel pin diode is described as an example of the method of manufacturing a semiconductor device, the semiconductor substrate of the present invention is further applicable to bipolar devices, Insulated Gate Bipolar Transistor (IGBT) devices, parasitic diodes of a Metal Oxide Semiconductor (MOS) structure, and the like. Further, in the embodiment, although an example has been described in which the n-type epitaxial layer 4, the n⁺-type silicon carbide buffer layer 2, and the n-type drift layer 3 are stacked on the front surface of the n⁺-type silicon carbide substrate 1, configuration may be such that a p-type epitaxial layer, a p⁺-type silicon carbide buffer layer, and a p-type drift layer are stacked on a front surface of a p⁺-type silicon carbide substrate.

As described, according to the silicon carbide semiconductor substrate of the embodiment, infrared light is reflected by the interface of the n⁺-type silicon carbide substrate and the n-type epitaxial layer, or the interface of the n-type epitaxial layer and the n⁺-type silicon carbide buffer layer and therefore, the film thickness of the n⁺-type silicon carbide buffer layer may be measured by Fourier transform from the interference waveform of the surface reflected light and the interface reflected light. Thus, it becomes possible to measure the thickness of the n⁺-type silicon carbide buffer layer by a conventional FT-IR method. As a result, for example, the film thickness of the n⁺-type silicon carbide buffer layer may be evaluated and managed, which may contribute to improved yield of the silicon carbide semiconductor substrate.

Further, the impurity concentration of the n-type epitaxial layer is ⅓ or less of the impurity concentration of the n⁺-type silicon carbide substrate or ⅓ or less of the impurity concentration of the n⁺-type silicon carbide buffer layer, whereby the reflected light at the interface becomes stronger, enabling the interference waveform of the surface reflected light and the interface reflected light to be obtained.

Further, the film thickness of the n-type epitaxial layer is 5 μm or less, whereby the resistance of the n-type epitaxial layer is suppressed, enabling increases in the resistance caused by the n-type epitaxial layer to be suppressed. Further, the impurity concentration of the n-type epitaxial layer is 1×10¹⁷/cm³ or higher, whereby the resistance of the n-type epitaxial layer is suppressed, enabling increases in the resistance caused by the n-type epitaxial layer to be suppressed.

According to the embodiments, stacking faults may be suppressed by the impurity concentration and thickness of the buffer layer. Further, since infrared light is reflected by the interface of the silicon carbide substrate and the epitaxial layer or the interface of the epitaxial layer and the buffer layer, the thickness of the buffer layer may be measured from the interference waveform of the surface reflected light and the interface reflected light by Fourier transform. Therefore, measurement of the thickness of the buffer layer by a conventional FT-IR method becomes possible. As a result, for example, the film thickness of the buffer layer may be evaluated and managed, which may contribute to improved yield of the silicon carbide semiconductor substrate.

Further, the impurity concentration of the epitaxial layer is ⅓ or less of the impurity concentration of the silicon carbide substrate or the buffer layer, whereby the reflected light at the interface becomes stronger, enabling an interference waveform of the surface reflected light and the interface reflected light to be obtained.

Further, the film thickness of the epitaxial layer is 5 μm or less, whereby the resistance of the epitaxial layer is suppressed, enabling increases in the resistance caused by the epitaxial layer to be suppressed. The impurity concentration of the epitaxial layer is 1×10¹⁷/cm³ or higher, whereby the resistance of the epitaxial layer is suppressed, enabling increases in the resistance caused by the epitaxial layer to be suppressed.

The silicon carbide semiconductor substrate, the method of manufacturing a silicon carbide semiconductor substrate, the semiconductor device, and the method of manufacturing a semiconductor device according to the embodiments achieve an effect in that even when a buffer layer having an impurity concentration that is about the same as that of the substrate is used to suppress stacking faults, the film thickness of the buffer layer may be measured by a conventional FT-IR method.

As described, the semiconductor substrate according to the embodiments is useful for a semiconductor substrate of a high-voltage semiconductor device used in power converting equipment and power supply devices such as in various industrial machines.

Although the invention has been described with respect to a specific embodiment for a complete and clear disclosure, the appended claims are not to be thus limited but are to be construed as embodying all modifications and alternative constructions that may occur to one skilled in the art which fairly fall within the basic teaching herein set forth. 

What is claimed is:
 1. A silicon carbide semiconductor substrate comprising: a silicon carbide substrate of a first conductivity type; an epitaxial layer of the first conductivity type provided on a front surface of the silicon carbide substrate, an impurity concentration of the epitaxial layer being 1×10¹⁷/cm³ to 1×10¹⁸/cm³, and a film thickness of the epitaxial layer being 1 μm to 5 μm; a buffer layer of the first conductivity type provided on a surface of a first side of the epitaxial layer opposite a second side facing the silicon carbide substrate, an impurity concentration of the buffer layer being about a same impurity concentration as an impurity concentration of the silicon carbide substrate, the impurity concentration of the buffer layer being at least three times the impurity concentration of the epitaxial layer, and a thickness of the buffer layer being at least 3 μm; and a drift layer of the first conductivity type provided on a surface of a first side of the buffer layer opposite a second side facing toward the silicon carbide substrate, an impurity concentration of the drift layer being lower than the impurity concentration of the buffer layer.
 2. A semiconductor device comprising a silicon carbide semiconductor substrate that includes: a silicon carbide substrate of a first conductivity type; an epitaxial layer of the first conductivity type provided on a front surface of the silicon carbide substrate, an impurity concentration of the epitaxial layer being 1×10¹⁷/cm³ to 1×10¹⁸/cm³, and a film thickness of the epitaxial layer being 1 μm to 5 μm; a buffer layer of the first conductivity type provided on a surface of a first side of the epitaxial layer opposite a second side facing the silicon carbide substrate, an impurity concentration of the buffer layer being about a same impurity concentration as an impurity concentration of the silicon carbide substrate, the impurity concentration of the buffer layer being at least three times the impurity concentration of the epitaxial layer, and a thickness of the buffer layer being at least 3 μm; and a drift layer of the first conductivity type provided on a surface of a first side of the buffer layer opposite a second side facing toward the silicon carbide substrate, an impurity concentration of the drift layer being lower than the impurity concentration of the buffer layer. 